Using the entire out-of-equilibrium distribution function upto first order, the dissipative currents can be written as [1]}, [2]}, [3]}
\(&\delta n^{(1)}, \delta \epsilon ^{(1)}, \delta P^{(1)}=\nu _{1},\varepsilon _{1},\pi _{1} \frac{\dot{T}}{T} + \nu _{2} ,\varepsilon _{2},\pi _{2}\left(\partial \cdot u\right)+\nu _{3},\varepsilon _{3},\pi _{3} \dot{\tilde{\mu }}~,\\&W^{(1)\mu },V^{(1)\mu } = \theta _{1},\gamma _{1}\left[\frac{\nabla ^{\mu }T}{T} - \dot{u}^{\mu }\right] +\theta _{3},\gamma _{3} \nabla ^{\mu }\tilde{\mu }~.\) 
